US20220128651A1 - Phase-tracking self-injection-locked radar - Google Patents
Phase-tracking self-injection-locked radar Download PDFInfo
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- US20220128651A1 US20220128651A1 US17/106,315 US202017106315A US2022128651A1 US 20220128651 A1 US20220128651 A1 US 20220128651A1 US 202017106315 A US202017106315 A US 202017106315A US 2022128651 A1 US2022128651 A1 US 2022128651A1
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/02—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
- G01S7/35—Details of non-pulse systems
- G01S7/352—Receivers
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L7/00—Automatic control of frequency or phase; Synchronisation
- H03L7/06—Automatic control of frequency or phase; Synchronisation using a reference signal applied to a frequency- or phase-locked loop
- H03L7/08—Details of the phase-locked loop
- H03L7/099—Details of the phase-locked loop concerning mainly the controlled oscillator of the loop
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/02—Systems using reflection of radio waves, e.g. primary radar systems; Analogous systems
- G01S13/50—Systems of measurement based on relative movement of target
- G01S13/58—Velocity or trajectory determination systems; Sense-of-movement determination systems
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/88—Radar or analogous systems specially adapted for specific applications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/02—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L7/00—Automatic control of frequency or phase; Synchronisation
- H03L7/06—Automatic control of frequency or phase; Synchronisation using a reference signal applied to a frequency- or phase-locked loop
- H03L7/08—Details of the phase-locked loop
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03L—AUTOMATIC CONTROL, STARTING, SYNCHRONISATION OR STABILISATION OF GENERATORS OF ELECTRONIC OSCILLATIONS OR PULSES
- H03L7/00—Automatic control of frequency or phase; Synchronisation
- H03L7/24—Automatic control of frequency or phase; Synchronisation using a reference signal directly applied to the generator
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/02—Systems using reflection of radio waves, e.g. primary radar systems; Analogous systems
- G01S13/50—Systems of measurement based on relative movement of target
Definitions
- This invention generally relates to a self-injection-locked (SIL) radar, and more particularly to a phase-tracking SIL radar.
- SIL self-injection-locked
- Continuous-wave (CW) Doppler radars are widely used to monitor vital signs of people or animals.
- SIL radar one of the conventional CW Doppler radars
- the conventional CW Doppler radars including the SIL radar for detecting vital signs are known to have optimal and null detection points.
- the optimal and null detection points occur alternatively every eighth wavelength where the maximum and minimum amplitudes of the detected vital signs are at the optimal and null detection points, respectively. Therefore, the conventional CW Doppler radars for monitoring vital signs often exhibit strong nonlinearity due to the amplitude dependence on the detected position when a target moves more than a quarter-wavelength during the monitoring period. This nonlinearity causes difficulties in tracking vital signs of the moving target with the conventional CW Doppler radars.
- the phase-tracking SIL radar of the present invention uses a phase-tracking SIL loop to automatically set the relative phases between the radar and the target to those of the optimal detection points, and thus can track vital signs of the moving target with high sensitivity and high linearity.
- phase-tracking SIL radar including an SIL oscillator, a phase-tracking SIL loop and a frequency-locked loop.
- the SIL oscillator generates an electrical oscillation signal and receives an electrical injection signal related to the electrical oscillation signal for self-injection locking.
- the phase-tracking SIL loop receives the electrical oscillation signal from the SIL oscillator and outputs the electrical injection signal to the SIL oscillator with a constant phase difference between the electrical oscillation signal and the electrical injection signal.
- the frequency-locked loop receives the electrical oscillation signal from the SIL oscillator and produces an electrical control signal to control the phase-tracking SIL loop or the SIL oscillator for eliminating the frequency shift of the SIL oscillator caused by the phase-tracking SIL loop. Accordingly, the phase difference between the electrical oscillation signal and the electrical injection signal is maintained at 0° or 180° such that the phase-tracking SIL radar operates at the optimal detection points.
- the phase-tracking SIL radar of the present invention differs from the conventional SIL radar by including the phase-tracking SIL loop and the frequency-locked loop to always operate at the optimal detection points. By doing so, its sensitivity and linearity are significantly improved for detection of vital signs when compared to those of the conventional SIL radar. As a result, the present invention can monitor vital signs of the target who can move more than a quarter-wavelength during the monitoring period.
- FIG. 1 is a block diagram illustrating a phase-tracking SIL radar of the present invention.
- FIG. 2 is a circuit diagram illustrating a phase-tracking SIL radar in accordance with a first embodiment of the present invention.
- FIG. 3 is a circuit diagram illustrating a frequency demodulator in accordance with the first embodiment of the present invention.
- FIG. 4 is a circuit diagram illustrating a phase-tracking SIL radar in accordance with a second embodiment of the present invention.
- FIG. 5 shows the measured displacement of a moving target using the phase-tracking SIL radar in accordance with the first embodiment of the present invention.
- FIG. 6 shows the spectrum of the measured data of FIG. 5 .
- FIG. 1 is a block diagram showing a phase-tracking SIL radar 100 of the present invention.
- the phase-tracking SIL radar 100 includes an SIL oscillator 110 , a phase-tracking SIL loop 120 and a frequency-locked loop 130 .
- the SIL oscillator 110 generates an electrical oscillation signal S osc and receives an electrical injection signal S inj related to the electrical oscillation signal S osc for self-injection locking.
- the phase-tracking SIL loop 120 is coupled to the SIL oscillator 110 to receive the electrical oscillation signal S osc from the SIL oscillator 110 and output the electrical injection signal S osc to the SIL oscillator 110 with a constant phase difference between the electrical oscillation signal S osc and the electrical injection signal S inj .
- the frequency-locked loop 130 is also coupled to the SIL oscillator 110 to receive and process the electrical oscillation signal S osc to produce an electrical control signal V c for controlling the phase-tracking SIL loop 120 or the SIL oscillator 110 to eliminate the frequency shift of the SIL oscillator 110 caused by the phase-tracking SIL loop 120 . Accordingly, the phase difference between the electrical oscillation signal S osc and the electrical injection signal S inj is maintained at 0° or 180° such that the phase-tracking SIL radar 100 operates at optimal detection points.
- FIG. 2 is a circuit diagram of a phase-tracking SIL radar 100 in accordance with a first embodiment of the present invention.
- the SIL oscillator 110 has an output port 111 for delivering the electrical oscillation signal S osc to the phase-tracking SIL loop 120 and the frequency-locked loop 130 and an injection port 112 for receiving the electrical injection signal S inj from the phase-tracking SIL loop 120 .
- the electrical injection signal S inj makes the SIL oscillator 110 enter an SIL state.
- the phase-tracking SIL loop 120 includes a transmitter 121 , a receiver 122 , a phase shifter 123 and a target 124 .
- the transmitter 121 is electrically connected to the SIL oscillator 110 to convert the electrical oscillation signal S osc from the SIL oscillator 110 into a wireless signal S w for transmission to the target 124 .
- the receiver 122 is provided to convert a reflected signal S r from the target 124 into the electrical injection signal S inj .
- the reflected signal S r and the wireless signal S w are in the same form of electromagnetic, acoustic or optical waves.
- the phase shifter 123 is electrically connected between the receiver 122 and the SIL oscillator 110 to phase-shift the electrical injection signal S inj for injection into the SIL oscillator 110 . Accordingly, the SIL oscillator 110 enters the SIL state. While a displacement ⁇ x of the target 124 relative to the transmitter 121 or the receiver 122 happens, the electrical injection signal S inj has a Doppler phase shift as a result of the Doppler effect on the reflected signal S r . Moreover, due to the phase-tracking SIL loop 120 , the frequency of the SIL oscillator 110 varies with the phase difference between the electrical oscillation signal S osc and the electrical injection signal S inj .
- the transmitter 121 and the receiver 122 may use electromagnetic antennas, acoustic transducers or optical transceivers for conversion between electrical signals and electromagnetic waves, acoustic waves or optical waves, respectively. Additionally, the transmitter 121 and the receiver 122 may include an amplifier and a frequency converter to amplify and frequency-convert the electrical oscillation signal S osc and the electrical injection signal S inj . Furthermore, the transmitter 121 and the receiver 122 may include a digital-to-analog converter (DAC) and an analog-to-digital converter (ADC) if the electrical oscillation signal S osc and the electrical injection signal S inj are digital signals.
- DAC digital-to-analog converter
- ADC analog-to-digital converter
- the frequency-locked loop 130 includes a frequency demodulator 131 and a controller 132 .
- the frequency demodulator 131 is electrically connected to the SIL oscillator 110 to demodulate the electrical oscillation signal S osc from the SIL oscillator 110 into an electrical frequency-shift signal ⁇ f.
- the controller 132 is electrically connected to the frequency demodulator 131 to produce an electrical control signal V c that depends on the electrical frequency-shift signal ⁇ f from the frequency demodulator 131 for delivery to the phase shifter 123 .
- the electrical control signal V c is used to control the phase shifter 123 to phase-shift the electrical injection signal S inj with the phase difference of 0° or 180° from the electrical oscillation signal S osc by eliminating the frequency shift of the SIL oscillator 110 caused by the phase-tracking SIL loop 120 .
- the frequency demodulator 131 in this embodiment includes a power splitter 131 a , a delay unit 131 b and a mixer 131 c .
- the power splitter 131 a is electrically connected to the output port 111 of the SIL oscillator 110 to split the electrical oscillation signal S osc from the output port 111 of the SIL oscillator 110 into two parts.
- the delay unit 131 b is electrically connected to the power splitter 131 a to delay one part of the electrical oscillation signal S osc from the power splitter 131 a and thus outputs an electrical delayed signal S de .
- the mixer 131 c is electrically connected to the power splitter 131 a and the delay unit 131 b to mix the other part of the electrical oscillation signal S osc from the power splitter 131 a with the electrical delayed signal S de from the delay unit 131 b and thus produces the electrical frequency-shift signal ⁇ f.
- f LR is a locking range of the SIL oscillator 110
- ⁇ d is the phase difference between the electrical oscillation signal S osc and the electrical injection signal S inj
- ⁇ p is the phase shift induced by the phase shifter 123
- d is the initial distance from the transmitter 121 or the receiver 122 to the target 124
- ⁇ is a wavelength of the wireless signal S w .
- ⁇ p is a change of the phase shift induced by the phase shifter 123 and K ⁇ is a phase-tuning sensitivity of the phase shifter 123 .
- the above equation indicates that the electrical control signal V c is proportional to the displacement ⁇ x of the target 124 .
- the displacement ⁇ x contains vital signs of the target 124 .
- the phase shifter 123 may be placed at other positions of the phase-tracking SIL loop 120 and controlled to phase-shift the electrical injection signal S inj or the electrical oscillation signal S osc for maintaining the phase difference of 0° or 180° between both signals.
- FIG. 4 is a circuit diagram of a phase-tracking SIL radar 100 of a second embodiment of the present invention.
- the SIL oscillator 110 further comprises a frequency control terminal 113 .
- the phase-tracking SIL loop 120 includes the transmitter 121 , the receiver 122 and the target 124 , and excludes the phase shifter 123 .
- the transmitter 121 is electrically connected to the SIL oscillator 110 to convert the electrical oscillation signal S osc from the SIL oscillator 110 into the wireless signal S w for transmission to the target 124 .
- the receiver 122 converts the reflected signal S r from the target 124 into the electrical injection signal S inj for injection into the SIL oscillator 110 .
- the frequency-locked loop 130 includes the frequency demodulator 131 and the controller 132 .
- the frequency demodulator 131 is electrically connected to the SIL oscillator 110 to demodulate the electrical oscillation signal S osc from the SIL oscillator 110 into the electrical frequency-shift signal ⁇ f.
- the controller 132 is electrically connected to the frequency demodulator 131 to produce the electrical control signal V c that depends on the electrical frequency-shift signal ⁇ f from the frequency demodulator 131 for delivery to the frequency control terminal 113 of the SIL oscillator 110 .
- the electrical control signal V c controls the SIL oscillator 110 to frequency-shift the electrical oscillation signal S osc with the phase difference of 0° or 180° from the electrical injection signal S inj by cancelling the electrical frequency-shift signal ⁇ f. Accordingly, the electrical control signal V c can be derived in steady state as
- f 0 and K v is an initial frequency and a frequency-tuning sensitivity of the SIL oscillator 110 , respectively, and the plus and minus sign corresponds to the phase difference of 0° and 180°, respectively, between the electrical oscillation signal S osc and the electrical injection signal S inj .
- the above equation indicates that the electrical control signal V c is proportional to the displacement ⁇ x of the target 124 .
- the displacement ⁇ x contains vital signs of the target 124 .
- FIG. 5 shows the result of using the phase-tracking SIL radar 100 of the first embodiment to measure chest movements of a subject seated 30 cm from the radar.
- the wireless signal S w transmitted from the phase-tracking SIL radar 100 is an ultrasonic wave with a frequency of 40 kHz and a wavelength ( ⁇ ) of 8.6 mm.
- the measured result shown in FIG. 5 includes the small back and forth body movements and tiny movements due to vital signs.
- FIG. 6 is the spectrum of the measured data presented in FIG. 6 where the arrows point at the respiratory movements, body movements and heartbeat with the frequencies of 0.21, 0.82 and 1.42 Hz, respectively.
- phase-tracking SIL radar 100 of the present invention can overcome the nonlinearity arising from the body movements and is therefore suitable for monitoring vital signs of the moving subject.
- the phase-tracking SIL radar 100 of the present invention differs from the conventional SIL radar by including the phase-tracking SIL loop 120 and the frequency-locked loop 130 to always operate at the optimal detection points. By doing so, its sensitivity and linearity are significantly improved for detection of vital signs when compared to those of the conventional SIL radar. As a result, the present invention can monitor vital signs of the target 124 who can move more than a quarter-wavelength during the monitoring period.
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Abstract
Description
- This invention generally relates to a self-injection-locked (SIL) radar, and more particularly to a phase-tracking SIL radar.
- Continuous-wave (CW) Doppler radars are widely used to monitor vital signs of people or animals. In recent years, SIL radar, one of the conventional CW Doppler radars, has received increasing attention because of its extraordinarily high sensitivity of vital sign detection. However, the conventional CW Doppler radars including the SIL radar for detecting vital signs are known to have optimal and null detection points. The optimal and null detection points occur alternatively every eighth wavelength where the maximum and minimum amplitudes of the detected vital signs are at the optimal and null detection points, respectively. Therefore, the conventional CW Doppler radars for monitoring vital signs often exhibit strong nonlinearity due to the amplitude dependence on the detected position when a target moves more than a quarter-wavelength during the monitoring period. This nonlinearity causes difficulties in tracking vital signs of the moving target with the conventional CW Doppler radars.
- The phase-tracking SIL radar of the present invention uses a phase-tracking SIL loop to automatically set the relative phases between the radar and the target to those of the optimal detection points, and thus can track vital signs of the moving target with high sensitivity and high linearity.
- One aspect of the present invention provides a phase-tracking SIL radar including an SIL oscillator, a phase-tracking SIL loop and a frequency-locked loop. The SIL oscillator generates an electrical oscillation signal and receives an electrical injection signal related to the electrical oscillation signal for self-injection locking. The phase-tracking SIL loop receives the electrical oscillation signal from the SIL oscillator and outputs the electrical injection signal to the SIL oscillator with a constant phase difference between the electrical oscillation signal and the electrical injection signal. The frequency-locked loop receives the electrical oscillation signal from the SIL oscillator and produces an electrical control signal to control the phase-tracking SIL loop or the SIL oscillator for eliminating the frequency shift of the SIL oscillator caused by the phase-tracking SIL loop. Accordingly, the phase difference between the electrical oscillation signal and the electrical injection signal is maintained at 0° or 180° such that the phase-tracking SIL radar operates at the optimal detection points.
- The phase-tracking SIL radar of the present invention differs from the conventional SIL radar by including the phase-tracking SIL loop and the frequency-locked loop to always operate at the optimal detection points. By doing so, its sensitivity and linearity are significantly improved for detection of vital signs when compared to those of the conventional SIL radar. As a result, the present invention can monitor vital signs of the target who can move more than a quarter-wavelength during the monitoring period.
-
FIG. 1 is a block diagram illustrating a phase-tracking SIL radar of the present invention. -
FIG. 2 is a circuit diagram illustrating a phase-tracking SIL radar in accordance with a first embodiment of the present invention. -
FIG. 3 is a circuit diagram illustrating a frequency demodulator in accordance with the first embodiment of the present invention. -
FIG. 4 is a circuit diagram illustrating a phase-tracking SIL radar in accordance with a second embodiment of the present invention. -
FIG. 5 shows the measured displacement of a moving target using the phase-tracking SIL radar in accordance with the first embodiment of the present invention. -
FIG. 6 shows the spectrum of the measured data ofFIG. 5 . -
FIG. 1 is a block diagram showing a phase-tracking SIL radar 100 of the present invention. The phase-tracking SIL radar 100 includes anSIL oscillator 110, a phase-tracking SIL loop 120 and a frequency-lockedloop 130. TheSIL oscillator 110 generates an electrical oscillation signal Sosc and receives an electrical injection signal Sinj related to the electrical oscillation signal Sosc for self-injection locking. The phase-tracking SIL loop 120 is coupled to theSIL oscillator 110 to receive the electrical oscillation signal Sosc from theSIL oscillator 110 and output the electrical injection signal Sosc to theSIL oscillator 110 with a constant phase difference between the electrical oscillation signal Sosc and the electrical injection signal Sinj. The frequency-lockedloop 130 is also coupled to theSIL oscillator 110 to receive and process the electrical oscillation signal Sosc to produce an electrical control signal Vc for controlling the phase-tracking SIL loop 120 or theSIL oscillator 110 to eliminate the frequency shift of theSIL oscillator 110 caused by the phase-tracking SIL loop 120. Accordingly, the phase difference between the electrical oscillation signal Sosc and the electrical injection signal Sinj is maintained at 0° or 180° such that the phase-tracking SIL radar 100 operates at optimal detection points. -
FIG. 2 is a circuit diagram of a phase-tracking SIL radar 100 in accordance with a first embodiment of the present invention. In this embodiment, theSIL oscillator 110 has anoutput port 111 for delivering the electrical oscillation signal Sosc to the phase-tracking SIL loop 120 and the frequency-lockedloop 130 and aninjection port 112 for receiving the electrical injection signal Sinj from the phase-tracking SIL loop 120. The electrical injection signal Sinj makes theSIL oscillator 110 enter an SIL state. - The phase-
tracking SIL loop 120 includes atransmitter 121, areceiver 122, aphase shifter 123 and atarget 124. Thetransmitter 121 is electrically connected to theSIL oscillator 110 to convert the electrical oscillation signal Sosc from theSIL oscillator 110 into a wireless signal Sw for transmission to thetarget 124. Thereceiver 122 is provided to convert a reflected signal Sr from thetarget 124 into the electrical injection signal Sinj. The reflected signal Sr and the wireless signal Sw are in the same form of electromagnetic, acoustic or optical waves. - The
phase shifter 123 is electrically connected between thereceiver 122 and theSIL oscillator 110 to phase-shift the electrical injection signal Sinj for injection into theSIL oscillator 110. Accordingly, theSIL oscillator 110 enters the SIL state. While a displacement Δx of thetarget 124 relative to thetransmitter 121 or thereceiver 122 happens, the electrical injection signal Sinj has a Doppler phase shift as a result of the Doppler effect on the reflected signal Sr. Moreover, due to the phase-tracking SIL loop 120, the frequency of theSIL oscillator 110 varies with the phase difference between the electrical oscillation signal Sosc and the electrical injection signal Sinj. - The
transmitter 121 and thereceiver 122 may use electromagnetic antennas, acoustic transducers or optical transceivers for conversion between electrical signals and electromagnetic waves, acoustic waves or optical waves, respectively. Additionally, thetransmitter 121 and thereceiver 122 may include an amplifier and a frequency converter to amplify and frequency-convert the electrical oscillation signal Sosc and the electrical injection signal Sinj. Furthermore, thetransmitter 121 and thereceiver 122 may include a digital-to-analog converter (DAC) and an analog-to-digital converter (ADC) if the electrical oscillation signal Sosc and the electrical injection signal Sinj are digital signals. - With reference to
FIG. 2 , the frequency-lockedloop 130 includes afrequency demodulator 131 and acontroller 132. Thefrequency demodulator 131 is electrically connected to theSIL oscillator 110 to demodulate the electrical oscillation signal Sosc from theSIL oscillator 110 into an electrical frequency-shift signal Δf. Thecontroller 132 is electrically connected to thefrequency demodulator 131 to produce an electrical control signal Vc that depends on the electrical frequency-shift signal Δf from thefrequency demodulator 131 for delivery to thephase shifter 123. The electrical control signal Vc is used to control thephase shifter 123 to phase-shift the electrical injection signal Sinj with the phase difference of 0° or 180° from the electrical oscillation signal Sosc by eliminating the frequency shift of theSIL oscillator 110 caused by the phase-tracking SIL loop 120. - With reference to
FIG. 3 , thefrequency demodulator 131 in this embodiment includes apower splitter 131 a, adelay unit 131 b and amixer 131 c. Thepower splitter 131 a is electrically connected to theoutput port 111 of theSIL oscillator 110 to split the electrical oscillation signal Sosc from theoutput port 111 of theSIL oscillator 110 into two parts. Thedelay unit 131 b is electrically connected to thepower splitter 131 a to delay one part of the electrical oscillation signal Sosc from thepower splitter 131 a and thus outputs an electrical delayed signal Sde. Themixer 131 c is electrically connected to thepower splitter 131 a and thedelay unit 131 b to mix the other part of the electrical oscillation signal Sosc from thepower splitter 131 a with the electrical delayed signal Sde from thedelay unit 131 b and thus produces the electrical frequency-shift signal Δf. - The relation of the electrical frequency-shift signal Δf to the displacement Δx of the
target 124 is modeled by the following equation: -
- where fLR is a locking range of the
SIL oscillator 110, θd is the phase difference between the electrical oscillation signal Sosc and the electrical injection signal Sinj, θp is the phase shift induced by thephase shifter 123, d is the initial distance from thetransmitter 121 or thereceiver 122 to thetarget 124, and λ is a wavelength of the wireless signal Sw. The above equation indicates that the phase difference between the electrical oscillation signal Sosc and the electrical injection signal Sinj can be set to 0° or 180° (i.e. θd=2nπ or nπ, n=integer) by eliminating the frequency shift of the SIL oscillator 110 (i.e. Δf=0). Accordingly, the electrical control signal Vc can be estimated in steady state as -
- where Δθp is a change of the phase shift induced by the
phase shifter 123 and Kθ is a phase-tuning sensitivity of thephase shifter 123. The above equation indicates that the electrical control signal Vc is proportional to the displacement Δx of thetarget 124. As thetarget 124 is a person or an animal, the displacement Δx contains vital signs of thetarget 124. - The
phase shifter 123 may be placed at other positions of the phase-tracking SIL loop 120 and controlled to phase-shift the electrical injection signal Sinj or the electrical oscillation signal Sosc for maintaining the phase difference of 0° or 180° between both signals. -
FIG. 4 is a circuit diagram of a phase-tracking SIL radar 100 of a second embodiment of the present invention. In this embodiment, theSIL oscillator 110 further comprises afrequency control terminal 113. The phase-trackingSIL loop 120 includes thetransmitter 121, thereceiver 122 and thetarget 124, and excludes thephase shifter 123. Thetransmitter 121 is electrically connected to theSIL oscillator 110 to convert the electrical oscillation signal Sosc from theSIL oscillator 110 into the wireless signal Sw for transmission to thetarget 124. Thereceiver 122 converts the reflected signal Sr from thetarget 124 into the electrical injection signal Sinj for injection into theSIL oscillator 110. - With reference to
FIG. 4 , the frequency-lockedloop 130 includes thefrequency demodulator 131 and thecontroller 132. Thefrequency demodulator 131 is electrically connected to theSIL oscillator 110 to demodulate the electrical oscillation signal Sosc from theSIL oscillator 110 into the electrical frequency-shift signal Δf. Thecontroller 132 is electrically connected to thefrequency demodulator 131 to produce the electrical control signal Vc that depends on the electrical frequency-shift signal Δf from thefrequency demodulator 131 for delivery to thefrequency control terminal 113 of theSIL oscillator 110. In order to operate the phase-trackingSIL radar 100 at the optimal detection points, the electrical control signal Vc controls theSIL oscillator 110 to frequency-shift the electrical oscillation signal Sosc with the phase difference of 0° or 180° from the electrical injection signal Sinj by cancelling the electrical frequency-shift signal Δf. Accordingly, the electrical control signal Vc can be derived in steady state as -
- where f0 and Kv is an initial frequency and a frequency-tuning sensitivity of the
SIL oscillator 110, respectively, and the plus and minus sign corresponds to the phase difference of 0° and 180°, respectively, between the electrical oscillation signal Sosc and the electrical injection signal Sinj. The above equation indicates that the electrical control signal Vc is proportional to the displacement Δx of thetarget 124. As thetarget 124 is the person or the animal, the displacement Δx contains vital signs of thetarget 124. -
FIG. 5 shows the result of using the phase-trackingSIL radar 100 of the first embodiment to measure chest movements of a subject seated 30 cm from the radar. The wireless signal Sw transmitted from the phase-trackingSIL radar 100 is an ultrasonic wave with a frequency of 40 kHz and a wavelength (λ) of 8.6 mm. The measured result shown inFIG. 5 includes the small back and forth body movements and tiny movements due to vital signs.FIG. 6 is the spectrum of the measured data presented inFIG. 6 where the arrows point at the respiratory movements, body movements and heartbeat with the frequencies of 0.21, 0.82 and 1.42 Hz, respectively. Moreover, the nonlinear artifacts caused by the body movements with an amplitude of 4.5 mm (0.52λ) are quite low so not to overwhelm the vital sign movements. This result demonstrates that the phase-trackingSIL radar 100 of the present invention can overcome the nonlinearity arising from the body movements and is therefore suitable for monitoring vital signs of the moving subject. - The phase-tracking
SIL radar 100 of the present invention differs from the conventional SIL radar by including the phase-trackingSIL loop 120 and the frequency-lockedloop 130 to always operate at the optimal detection points. By doing so, its sensitivity and linearity are significantly improved for detection of vital signs when compared to those of the conventional SIL radar. As a result, the present invention can monitor vital signs of thetarget 124 who can move more than a quarter-wavelength during the monitoring period. - While this invention has been particularly illustrated and described in detail with respect to the preferred embodiments thereof, it will be clearly understood by those skilled in the art that is not limited to the specific features shown and described and various modified and changed in form and details may be made without departing from the spirit and scope of this invention.
Claims (13)
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| TW109136758 | 2020-10-22 | ||
| TW109136758A TWI744046B (en) | 2020-10-22 | 2020-10-22 | Phase-tracking self-injection-locked radar |
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| US20220128651A1 true US20220128651A1 (en) | 2022-04-28 |
| US11360189B2 US11360189B2 (en) | 2022-06-14 |
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| TWI780543B (en) * | 2020-12-18 | 2022-10-11 | 國立中山大學 | Frequency-converted frequency-modulated self-injection-locked radar |
| TWI776751B (en) * | 2021-12-10 | 2022-09-01 | 國立高雄師範大學 | System and method for detecting stimulated acupuncture point |
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| FR2681696B1 (en) * | 1988-11-07 | 1994-01-07 | Gec Marconi Ltd | RADAR SYSTEM USING AN INJECTION LOCKED TRANSMITTER STAGE. |
| US9603555B2 (en) * | 2010-05-17 | 2017-03-28 | Industrial Technology Research Institute | Motion/vibration detection system and method with self-injection locking |
| US9375153B2 (en) * | 2010-05-17 | 2016-06-28 | Industrial Technology Research Institute | Motion/vibration sensor |
| WO2012132847A1 (en) * | 2011-03-31 | 2012-10-04 | 国立大学法人東京工業大学 | Injection-locked type frequency-locked oscillator |
| US9109862B2 (en) * | 2011-05-24 | 2015-08-18 | Bird Aerosystems Limited | System, device, and method of protecting aircrafts against incoming threats |
| WO2013112955A1 (en) * | 2012-01-27 | 2013-08-01 | The Regents Of The University Of California | Sub-carrier successive approximation millimeter wave radar for high-accuracy 3d imaging |
| TWI616669B (en) * | 2017-02-07 | 2018-03-01 | 國立中山大學 | Orthogonal self-injection locking radar |
| TWI609192B (en) * | 2017-05-26 | 2017-12-21 | 國立中山大學 | Vital sign monitoring system |
| TWI642406B (en) * | 2017-12-12 | 2018-12-01 | Sil Radar Technology Inc. | Non-contact self-injection locking sensor |
| TWI675643B (en) * | 2018-05-31 | 2019-11-01 | 國立中山大學 | Non-contact pulse transit time measurement system and non-contact vital sign sensing device thereof |
| TWI675218B (en) * | 2018-06-07 | 2019-10-21 | 國立中山大學 | Vital sign sensor capable of resisting clutter |
| TWI677700B (en) * | 2018-07-17 | 2019-11-21 | 昇雷科技股份有限公司 | Doppler Radar with Power Detector |
| TWI743379B (en) * | 2018-07-18 | 2021-10-21 | 昇雷科技股份有限公司 | Vital sign signal detecting method of the vital sign detecting system and method for evaluating a confidence of the vital sign signal |
| TWI682649B (en) * | 2018-09-28 | 2020-01-11 | 國立中山大學 | Signal demodulation device with iq mixer and demodulated method thereof |
| TWI669913B (en) * | 2019-03-15 | 2019-08-21 | 昇雷科技股份有限公司 | Frequency-converted self-injection-locked radar |
| TWI696844B (en) * | 2019-04-26 | 2020-06-21 | 昇雷科技股份有限公司 | Six port self-injection locked radar |
| CN111289966B (en) * | 2020-02-20 | 2022-05-10 | 上海交通大学 | Motion Information Measurement Method Based on Coherent Phase Tracking of MIMO FMCW Radar |
| TWI723824B (en) * | 2020-03-30 | 2021-04-01 | 國立高雄科技大學 | Wireless frequency-locked-loop vital sign sensing radar |
| TWI719893B (en) * | 2020-04-29 | 2021-02-21 | 國立中山大學 | Digital self-injection-locked radar |
| TWI723873B (en) * | 2020-05-13 | 2021-04-01 | 國立中山大學 | Six-port self-injection-locked radar |
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| CN114389601B (en) | 2026-01-13 |
| US11360189B2 (en) | 2022-06-14 |
| CN114389601A (en) | 2022-04-22 |
| TWI744046B (en) | 2021-10-21 |
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